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Tanis, J.A.; Bernstein, E.M.; Clark, M.W.
Brookhaven National Lab., Upton, NY (USA); Western Michigan Univ., Kalamazoo (USA). Dept. of Physics; Ulster Univ., Coleraine (UK). Dept. of Physics; Missouri Univ., Rolla (USA). Dept. of Physics; Wesleyan Univ., Middletown, CT (USA). Dept. of Physics; Giessen Univ. (Germany, F.R.)1985
Brookhaven National Lab., Upton, NY (USA); Western Michigan Univ., Kalamazoo (USA). Dept. of Physics; Ulster Univ., Coleraine (UK). Dept. of Physics; Missouri Univ., Rolla (USA). Dept. of Physics; Wesleyan Univ., Middletown, CT (USA). Dept. of Physics; Giessen Univ. (Germany, F.R.)1985
AbstractAbstract
[en] In an ion-atom collision projectile excitation and charge transfer (electron capture) may occur together in a single encounter. If the excitation and capture are correlated, then the process is called resonant transfer and excitation (RTE); if they are uncorrelated, then the process is termed nonresonant transfer and excitation (NTE). Experimental work to date has shown the existence of RTE and provided strong evidence for NTE. Results presented here provide information on the relative magnitudes of RTE and NTE, the charge state dependence of RTE, the effect of the target momentum distribution on RTE, the magnitude of L-shell RTE compared to K-shell RTE, and the target Z dependences of RTE and NTE. 15 refs., 5 figs
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1985; 7 p; 14. international conference on the physics of electronic and atomic collisions; Palo Alto, CA (USA); 24-30 Jul 1985; CONF-850701--3; Available from NTIS, PC A02/MF A01 as DE86000030
Record Type
Report
Literature Type
Conference; Numerical Data
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